1981
DOI: 10.1029/jc086ic02p01205
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An efficient, accurate algorithm for calculating CO2 15 μm band cooling rates

Abstract: A fast, accurate method for obtaining atmospheric carbon dioxide transmission functions for the 15-/•m band is presented. Tables of transmissivities for CO2 mixing ratios of 330 and 660 ppmv on standard pressure grids comprising geopotential heights ranging from 0 to 80 km and using standard temperatures are included. An algorithm for interpolating from these values to any desired temperature profile and to any other pressure grid is detailed.

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Cited by 121 publications
(50 citation statements)
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References 26 publications
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“…In our LBL model, a four-point Gaussian quadrature method [Fels and Schwarzkopf, 1981] is used to perform the angular integration to obtain the OLR and DLR.…”
Section: Longwave Radiative Transfer Formulationmentioning
confidence: 99%
See 1 more Smart Citation
“…In our LBL model, a four-point Gaussian quadrature method [Fels and Schwarzkopf, 1981] is used to perform the angular integration to obtain the OLR and DLR.…”
Section: Longwave Radiative Transfer Formulationmentioning
confidence: 99%
“…Our analysis focuses on the Outgoing Longwave Radiation (OLR) at the Top of the Atmosphere (TOA) and Downward Longwave Radiation (DLR) at the surface under clear skies. We employ the Line-by-line (LBL) radiative transfer model of the Geophysical Fluid Dynamical Laboratory (GFDL) [Fels and Schwarzkopf, 1981;Schwarzkopf and Ramaswamy, 1999] for the computations.…”
Section: Introductionmentioning
confidence: 99%
“…With a view to understanding the interaction between model physics and aerosol radiative effects, we have conducted another set of simulations both with and without aerosol forcing and using the Kuo cumulus parameterization scheme (Anthes, 1977). The model's shortwave radiation scheme is based on Lacis and Hansen (1974) and the longwave radiation scheme is based on Fels and Schwarzkopf (1981). It uses a simple one layer bucket model for the surface hydrology calculation (Pan and Mahrt, 1986).…”
Section: Model Descriptionmentioning
confidence: 99%
“…Because a complete description of the present line-by-line model has been published elsewhere [Drayson, 1967;Fels and Schwarzkopf, 1981], only a brief review of its features will be outlined here. A few important differences in its use will also be noted.…”
Section: The Line-by-line Modelmentioning
confidence: 99%
“…Complete, selfconsistent numerical models of the thermal structures and dynamical states of these atmospheres therefore require reliable descriptions of the transmission within this band. The most versatile and accurate methods for finding this transmission are the line-by-line models, such as those described by Drayson [1967] and Fels and Schwarzkopf [1981]. These methods are called "exact," since they can employ all available information about absorption lines shapes, strengths, and positions, and their accuracy is limited primarily by uncertainties in these line parameters.…”
Section: Introductionmentioning
confidence: 99%